WO2015086258A1 - Source de rayonnement, appareil de métrologie, système lithographique et procédé de fabrication de dispositifs - Google Patents

Source de rayonnement, appareil de métrologie, système lithographique et procédé de fabrication de dispositifs Download PDF

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Publication number
WO2015086258A1
WO2015086258A1 PCT/EP2014/074659 EP2014074659W WO2015086258A1 WO 2015086258 A1 WO2015086258 A1 WO 2015086258A1 EP 2014074659 W EP2014074659 W EP 2014074659W WO 2015086258 A1 WO2015086258 A1 WO 2015086258A1
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WIPO (PCT)
Prior art keywords
radiation
container
plasma
source apparatus
radiation source
Prior art date
Application number
PCT/EP2014/074659
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English (en)
Inventor
Martijn Petrus Christianus VAN HEUMEN
Original Assignee
Asml Netherlands B.V.
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Asml Netherlands B.V. filed Critical Asml Netherlands B.V.
Priority to US15/103,721 priority Critical patent/US9924585B2/en
Priority to CN201480067916.7A priority patent/CN105814662B/zh
Priority to KR1020167018014A priority patent/KR101953712B1/ko
Publication of WO2015086258A1 publication Critical patent/WO2015086258A1/fr
Priority to IL245915A priority patent/IL245915B/en
Priority to US15/888,362 priority patent/US10420197B2/en

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Classifications

    • H—ELECTRICITY
    • H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
    • H05G—X-RAY TECHNIQUE
    • H05G2/00—Apparatus or processes specially adapted for producing X-rays, not involving X-ray tubes, e.g. involving generation of a plasma
    • H05G2/001—X-ray radiation generated from plasma
    • H05G2/008—X-ray radiation generated from plasma involving a beam of energy, e.g. laser or electron beam in the process of exciting the plasma
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/84—Systems specially adapted for particular applications
    • G01N21/88—Investigating the presence of flaws or contamination
    • G01N21/95—Investigating the presence of flaws or contamination characterised by the material or shape of the object to be examined
    • G01N21/9501—Semiconductor wafers
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/84—Systems specially adapted for particular applications
    • G01N21/88—Investigating the presence of flaws or contamination
    • G01N21/95—Investigating the presence of flaws or contamination characterised by the material or shape of the object to be examined
    • G01N21/956—Inspecting patterns on the surface of objects
    • G—PHYSICS
    • G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03F—PHOTOMECHANICAL PRODUCTION OF TEXTURED OR PATTERNED SURFACES, e.g. FOR PRINTING, FOR PROCESSING OF SEMICONDUCTOR DEVICES; MATERIALS THEREFOR; ORIGINALS THEREFOR; APPARATUS SPECIALLY ADAPTED THEREFOR
    • G03F7/00—Photomechanical, e.g. photolithographic, production of textured or patterned surfaces, e.g. printing surfaces; Materials therefor, e.g. comprising photoresists; Apparatus specially adapted therefor
    • G03F7/70—Microphotolithographic exposure; Apparatus therefor
    • G03F7/70058—Mask illumination systems
    • G03F7/70191—Optical correction elements, filters or phase plates for controlling intensity, wavelength, polarisation, phase or the like
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J61/00—Gas-discharge or vapour-discharge lamps
    • H01J61/02—Details
    • H01J61/30—Vessels; Containers
    • H01J61/35—Vessels; Containers provided with coatings on the walls thereof; Selection of materials for the coatings
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J61/00—Gas-discharge or vapour-discharge lamps
    • H01J61/02—Details
    • H01J61/54—Igniting arrangements, e.g. promoting ionisation for starting
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J61/00—Gas-discharge or vapour-discharge lamps
    • H01J61/02—Details
    • H01J61/54—Igniting arrangements, e.g. promoting ionisation for starting
    • H01J61/545—Igniting arrangements, e.g. promoting ionisation for starting using an auxiliary electrode inside the vessel
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J65/00—Lamps without any electrode inside the vessel; Lamps with at least one main electrode outside the vessel
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J65/00—Lamps without any electrode inside the vessel; Lamps with at least one main electrode outside the vessel
    • H01J65/04—Lamps in which a gas filling is excited to luminesce by an external electromagnetic field or by external corpuscular radiation, e.g. for indicating plasma display panels

Definitions

  • the present invention relates to plasma based radiation sources (photon
  • Such sources may be used for example to provide high brightness illumination in methods and for metrology usable, for example, in the manufacture of devices by lithographic techniques and to methods of manufacturing devices using lithographic techniques.
  • Radiation sources according to the invention may find application in a wide range of situations.
  • the following will describe use of the invention as a light source in metrology.
  • the following shall refer for the sake of example to metrology in the manufacture of devices by lithography.
  • the terms 'light' and 'light source' may be used conveniently to refer to the generated radiation and the radiation (or photon) source itself, without implying any limitation to radiation of visible wavelengths.
  • a lithographic apparatus is a machine that applies a desired pattern onto a substrate, usually onto a target portion of the substrate.
  • a lithographic apparatus can be used, for example, in the manufacture of integrated circuits (ICs).
  • a patterning device which is alternatively referred to as a mask or a reticle, may be used to generate a circuit pattern to be formed on an individual layer of the IC.
  • This pattern can be transferred onto a target portion (e.g., including part of, one, or several dies) on a substrate (e.g., a silicon wafer). Transfer of the pattern is typically via imaging onto a layer of radiation- sensitive material (resist) provided on the substrate.
  • a single substrate will contain a network of adjacent target portions that are successively patterned.
  • lithographic apparatus include so-called steppers, in which each target portion is irradiated by exposing an entire pattern onto the target portion at one time, and so-called scanners, in which each target portion is irradiated by scanning the pattern through a radiation beam in a given direction (the "scanning"- direction) while synchronously scanning the substrate parallel or anti parallel to this direction. It is also possible to transfer the pattern from the patterning device to the substrate by imprinting the pattern onto the substrate.
  • the light source is a xenon
  • (Xe) arc-discharge lamp Light from this lamp is imaged onto the measurement target through an illumination branch of the apparatus sensor, the last stage of which consists of a high-NA objective.
  • the measurement spot may have a diameter of 25 ⁇ , for example.
  • the time required for each measurement depends in practice on the brightness of the light source at a given wavelength or wave range. Future generations of apparatus are desired to provide an increased spectral bandwidth and sensor design with lower transmittance, while keeping the measurement time the same or shorter. Significant source brightness improvements are necessary to fulfill these requirements.
  • Plasma-based radiation (photon) sources for example laser driven light
  • LDLS LDLS
  • Plasmas are generated in a gaseous medium by the application of energy through electric discharge, and laser energy.
  • the spectral distribution of the radiation may be broadband or narrowband in nature, and wavelengths may be in the near infrared, visible and/or ultraviolet (UV) bands.
  • Published patent application US 2011/204265 Al discloses plasma based light sources including laser driven light sources directed at producing output radiation (at least partly) in the UV band.
  • One of the difficulties with LDLS is the short lifetime of the xenon arc-discharge bulbs used.
  • a radiation source apparatus comprising: a container for being pressurised with a gaseous medium in which plasma which emits plasma emitted radiation is generated following excitation of the gaseous medium by a driving radiation, wherein said container is operable substantially to remove radiation with a wavelength of 10-400 nm from said plasma emitted radiation before said plasma emitted radiation exits said container as output radiation.
  • apparatus comprising: a container for being pressurised with a gaseous medium in which plasma which emits plasma emitted radiation is generated following excitation of the gaseous medium by a driving radiation, said container comprising: an inlet radiation transmitting element operable to transmit said driving radiation from outside said container to inside said container, and an outlet radiation transmitting element operable to transmit at least some of said plasma emitted radiation from inside said container to outside said container as output radiation; wherein at least one of said inlet and outlet radiation transmitting elements comprises a plane parallel plate.
  • a container for being pressurised with a gaseous medium in which plasma which emits plasma emitted radiation is generated following excitation of the gaseous medium by a driving radiation said container comprising: an inlet radiation transmitting element operable to transmit said driving radiation from outside said container to inside said container, and an outlet radiation transmitting element operable to transmit at least some of said plasma emitted radiation from inside said container to outside said container as output radiation;
  • the radiation source may be applied in metrology, for example in lithography.
  • the invention in another aspect provides method of measuring a property of structures that have been formed by a lithographic process on a substrate, the method comprising the steps of:
  • the invention yet further provides an inspection apparatus for measuring a property of a structure on a substrate, the apparatus comprising: a support for the substrate having said structure thereon; an optical system for illuminating the structure under predetermined illumination conditions and for detecting predetermined portions of radiation diffracted by the component target structures under said illumination conditions; a processor arranged to process information characterizing the detected radiation to obtain a measurement of said property of the structure, wherein said optical system includes a radiation source apparatus according to the invention as set forth above.
  • the invention yet further provides a lithographic system comprising: a
  • lithographic apparatus comprising: an illumination optical system arranged to illuminate a pattern; a projection optical system arranged to project an image of the pattern onto a substrate; and an inspection apparatus according to an embodiment of the invention as set forth above, wherein the lithographic apparatus is arranged to use the measurement results from the inspection apparatus in applying the pattern to further substrates.
  • the invention yet further provides a method of manufacturing devices wherein a device pattern is applied to a series of substrates using a lithographic process, the method including inspecting at least one composite target structure formed as part of or beside said device pattern on at least one of said substrates using the
  • Figure 1 depicts a lithographic apparatus according to an embodiment of the invention
  • Figure 2 depicts a lithographic cell or cluster according to an embodiment of the invention
  • Figure 3 comprises a schematic diagram of an optical apparatus incorporating a photon source, the apparatus in this example having the form of a scatterometer used in metrology;
  • Figure 4 is a schematic diagram of a radiation source used in the apparatus of Figure 3.
  • Figure 5 is a schematic diagram of a radiation source apparatus, according to an embodiment of the present invention.
  • FIG. 1 schematically depicts a lithographic apparatus LA.
  • the apparatus includes an illumination system (illuminator) IL configured to condition a radiation beam B (e.g., UV radiation or DUV radiation), a patterning device support or support structure (e.g., a mask table) MT constructed to support a patterning device (e.g., a mask) MA and connected to a first positioner PM configured to accurately position the patterning device in accordance with certain parameters; a substrate table (e.g., a wafer table) WT constructed to hold a substrate (e.g., a resist coated wafer) W and connected to a second positioner PW configured to accurately position the substrate in accordance with certain parameters; and a projection system (e.g., a refractive projection lens system) PS configured to project a pattern imparted to the radiation beam B by patterning device MA onto a target portion C (e.g., including one or more dies) of the substrate W.
  • a radiation beam B e.g.
  • the illumination system may include various types of optical components, such as refractive, reflective, magnetic, electromagnetic, electrostatic or other types of optical components, or any combination thereof, for directing, shaping, or controlling radiation.
  • optical components such as refractive, reflective, magnetic, electromagnetic, electrostatic or other types of optical components, or any combination thereof, for directing, shaping, or controlling radiation.
  • the patterning device support holds the patterning device in a manner that depends on the orientation of the patterning device, the design of the lithographic apparatus, and other conditions, such as for example whether or not the patterning device is held in a vacuum environment.
  • the patterning device support can use mechanical, vacuum, electrostatic or other clamping techniques to hold the patterning device.
  • the patterning device support may be a frame or a table, for example, which may be fixed or movable as required.
  • the patterning device support may ensure that the patterning device is at a desired position, for example with respect to the projection system. Any use of the terms "reticle” or “mask” herein may be considered synonymous with the more general term "patterning device.”
  • patterning device used herein should be broadly interpreted as referring to any device that can be used to impart a radiation beam with a pattern in its cross-section such as to create a pattern in a target portion of the substrate. It should be noted that the pattern imparted to the radiation beam may not exactly correspond to the desired pattern in the target portion of the substrate, for example if the pattern includes phase- shifting features or so called assist features. Generally, the pattern imparted to the radiation beam will correspond to a particular functional layer in a device being created in the target portion, such as an integrated circuit.
  • the patterning device may be transmissive or reflective. Examples of
  • patterning devices include masks, programmable mirror arrays, and programmable LCD panels.
  • Masks are well known in lithography, and include mask types such as binary, alternating phase-shift, and attenuated phase-shift, as well as various hybrid mask types.
  • An example of a programmable mirror array employs a matrix arrangement of small mirrors, each of which can be individually tilted so as to reflect an incoming radiation beam in different directions. The tilted mirrors impart a pattern in a radiation beam, which is reflected by the mirror matrix.
  • projection system used herein should be broadly interpreted as encompassing any type of projection system, including refractive, reflective, catadioptric, magnetic, electromagnetic and electrostatic optical systems, or any combination thereof, as appropriate for the exposure radiation being used, or for other factors such as the use of an immersion liquid or the use of a vacuum. Any use of the term “projection lens” herein may be considered as synonymous with the more general term “projection system”.
  • the apparatus is of a transmissive type (e.g., employing a transmissive mask).
  • the apparatus may be of a reflective type (e.g., employing a programmable mirror array of a type as referred to above, or employing a reflective mask).
  • the lithographic apparatus may be of a type having two (dual stage) or more substrate tables (and/or two or more mask tables). In such "multiple stage” machines the additional tables may be used in parallel, or preparatory steps may be carried out on one or more tables while one or more other tables are being used for exposure.
  • the lithographic apparatus may also be of a type wherein at least a portion of the substrate may be covered by a liquid having a relatively high refractive index, e.g., water, so as to fill a space between the projection system and the substrate.
  • a liquid having a relatively high refractive index e.g., water
  • An immersion liquid may also be applied to other spaces in the lithographic apparatus, for example, between the mask and the projection system. Immersion techniques are well known in the art for increasing the numerical aperture of projection systems.
  • immersion as used herein does not mean that a structure, such as a substrate, must be submerged in liquid, but rather only means that liquid is located between the projection system and the substrate during exposure.
  • the illuminator IL receives a radiation beam from a radiation source SO.
  • the source and the lithographic apparatus may be separate entities, for example when the source is an excimer laser. In such cases, the source is not considered to form part of the lithographic apparatus and the radiation beam is passed from the source SO to the illuminator IL with the aid of a beam delivery system BD including, for example, suitable directing mirrors and/or a beam expander.
  • the source may be an integral part of the lithographic apparatus, for example when the source is a mercury lamp.
  • the source SO and the illuminator IL, together with the beam delivery system BD if required, may be referred to as a radiation system.
  • the illuminator IL may include an adjuster AD for adjusting the angular intensity distribution of the radiation beam. Generally, at least the outer and/or inner radial extent (commonly referred to as ⁇ -outer and ⁇ -inner, respectively) of the intensity distribution in a pupil plane of the illuminator can be adjusted.
  • the illuminator IL may include various other components, such as an integrator IN and a condenser CO. The illuminator may be used to condition the radiation beam, to have a desired uniformity and intensity distribution in its cross section.
  • the radiation beam B is incident on the patterning device (e.g., mask) MA, which is held on the patterning device support (e.g., mask table MT), and is patterned by the patterning device. Having traversed the patterning device (e.g., mask) MA, the radiation beam B passes through the projection system PS, which focuses the beam onto a target portion C of the substrate W.
  • the substrate table WT can be moved accurately, e.g., so as to position different target portions C in the path of the radiation beam B.
  • the first positioner PM and another position sensor can be used to accurately position the patterning device (e.g., mask) MA with respect to the path of the radiation beam B, e.g., after mechanical retrieval from a mask library, or during a scan.
  • movement of the patterning device support (e.g., mask table) MT may be realized with the aid of a long-stroke module (coarse positioning) and a short-stroke module (fine positioning), which form part of the first positioner PM.
  • movement of the substrate table WT may be realized using a long-stroke module and a short-stroke module, which form part of the second positioner PW.
  • the patterning device support (e.g., mask table) MT may be connected to a short-stroke actuator only, or may be fixed.
  • Patterning device (e.g., mask) MA and substrate W may be aligned using mask alignment marks Ml, M2 and substrate alignment marks PI, P2.
  • the substrate alignment marks as illustrated occupy dedicated target portions, they may be located in spaces between target portions (these are known as scribe-lane alignment marks).
  • the mask alignment marks may be located between the dies.
  • Small alignment markers may also be included within dies, in amongst the device features, in which case it is desirable that the markers be as small as possible and not require any different imaging or process conditions than adjacent features. The alignment system, which detects the alignment markers, is described further below.
  • the depicted apparatus could be used in at least one of the following modes:
  • step mode the patterning device support (e.g., mask table) MT and the substrate table WT are kept essentially stationary, while an entire pattern imparted to the radiation beam is projected onto a target portion C at one time (i.e., a single static exposure).
  • the substrate table WT is then shifted in the X and/or Y direction so that a different target portion C can be exposed.
  • the maximum size of the exposure field limits the size of the target portion C imaged in a single static exposure.
  • the patterning device support (e.g., mask table) MT and the substrate table WT are scanned synchronously while a pattern imparted to the radiation beam is projected onto a target portion C (i.e., a single dynamic exposure).
  • the velocity and direction of the substrate table WT relative to the patterning device support (e.g., mask table) MT may be determined by the (de-)magnification and image reversal characteristics of the projection system PS.
  • the maximum size of the exposure field limits the width (in the non-scanning direction) of the target portion in a single dynamic exposure, whereas the length of the scanning motion determines the height (in the scanning direction) of the target portion.
  • the patterning device support (e.g., mask table) MT is kept essentially stationary holding a programmable patterning device, and the substrate table WT is moved or scanned while a pattern imparted to the radiation beam is projected onto a target portion C.
  • a pulsed radiation source is employed and the programmable patterning device is updated as required after each movement of the substrate table WT or in between successive radiation pulses during a scan.
  • This mode of operation can be readily applied to maskless lithography that utilizes programmable patterning device, such as a programmable mirror array of a type as referred to above.
  • Lithographic apparatus LA is of a so-called dual stage type which has two substrate tables WTa, WTb and two stations - an exposure station and a measurement station - between which the substrate tables can be exchanged. While one substrate on one substrate table is being exposed at the exposure station, another substrate can be loaded onto the other substrate table at the measurement station and various preparatory steps carried out.
  • the preparatory steps may include mapping the surface level of the substrate using a level sensor LS and measuring the position of alignment markers on the substrate using an alignment sensor AS. This enables a substantial increase in the throughput of the apparatus. If the position sensor IF is not capable of measuring the position of the substrate table while it is at the measurement station as well as at the exposure station, a second position sensor may be provided to enable the positions of the substrate table to be tracked at both stations.
  • the lithographic apparatus LA forms part of a lithographic cell LC, also sometimes referred to a lithocell or cluster, which also includes apparatus to perform pre- and post-exposure processes on a substrate.
  • spin coaters SC to deposit resist layers
  • developers DE to develop exposed resist
  • chill plates CH chill plates
  • bake plates BK A substrate handler, or robot, RO picks up substrates from input/output ports I/Ol, 1/02, moves them between the different process apparatus and delivers then to the loading bay LB of the lithographic apparatus.
  • These devices which are often collectively referred to as the track, are under the control of a track control unit TCU which is itself controlled by the supervisory control system SCS, which also controls the lithographic apparatus via lithography control unit LACU.
  • the different apparatus can be operated to maximize throughput and processing efficiency.
  • Figure 3 is a schematic diagram of an optical apparatus in the form of a scatterometer suitable for performing metrology in conjunction with the lithocell of Figure 2.
  • the apparatus may be used for measuring critical dimensions of features formed by lithography, measuring overlay between layers and the like.
  • a product feature or dedicated metrology target is formed on substrate W.
  • the apparatus may be a stand-alone device or incorporated in either the lithographic apparatus LA, e.g., at the measurement station, or the lithographic cell LC.
  • An optical axis, which has several branches throughout the apparatus, is represented by a dotted line O.
  • light emitted by source 11 is directed onto substrate W via a beam splitter 15 by an optical system comprising lenses 12, 14 and objective lens 16.
  • the angular range at which the radiation is incident on the substrate can be selected by defining a spatial intensity distribution in a plane that presents the spatial spectrum of the substrate plane, here referred to as a (conjugate) pupil plane.
  • a spatial intensity distribution in a plane that presents the spatial spectrum of the substrate plane here referred to as a (conjugate) pupil plane.
  • this can be done by inserting an aperture plate 13 of suitable form between lenses 12 and 14, in a plane which is a back-projected image of the objective lens pupil plane.
  • aperture plate 13 can have different forms, two of which are labeled 13N and 13S, allowing different illumination modes to be selected.
  • the illumination system in the illustrated example forms an off-axis illumination mode.
  • aperture plate 13N provides off-axis from a direction designated, for the sake of description only, as 'north'.
  • aperture plate 13S is used to provide similar illumination, but from an opposite direction, labeled 'south'.
  • Other modes of illumination are possible by using different apertures.
  • the rest of the pupil plane is desirably dark as any unnecessary light outside the desired illumination mode will interfere with the desired measurement signals.
  • At least the 0th and one of the -1 and +1 orders diffracted by the target on substrate W are collected by objective lens 16 and directed back through beam splitter 15.
  • a second beam splitter 17 divides the diffracted beams into two measurement branches.
  • optical system 18 forms a diffraction spectrum (pupil plane image) of the target on first sensor 19 (e.g. a CCD or CMOS sensor) using the zeroth and first order diffractive beams.
  • first sensor 19 e.g. a CCD or CMOS sensor
  • Each diffraction order hits a different point on the sensor, so that image processing can compare and contrast orders.
  • the pupil plane image captured by sensor 19 can be used for focusing the metrology apparatus and/or normalizing intensity measurements of the first order beam.
  • the pupil plane image can be used for many measurement purposes such as reconstruction.
  • optical system 20, 22 forms an image of the target on the substrate W on sensor 23 (e.g. a CCD or CMOS sensor).
  • sensor 23 e.g. a CCD or CMOS sensor.
  • an aperture stop 21 is provided in a plane that is conjugate to the pupil-plane. Aperture stop 21 functions to block the zeroth order diffracted beam so that the image of the target formed on sensor 23 is formed only from the -1 or +1 first order beam.
  • the image detected by sensor 23 is thus referred to as a 'dark-field' image. Note that the term 'image' is used here in a broad sense. An image of the grating lines as such will not be formed, if only one of the -1 and +1 orders is present.
  • the images captured by sensors 19 and 23 are output to image processor and controller PU, the function of which will depend on the particular type of
  • Figure 4 shows schematically the principal components of a laser-driven
  • the central component is a bulb 40, for example a glass capsule, containing a predetermined gaseous atmosphere.
  • the bulb 40 is an arc bulb designed for exciting gas in the bulb by ionizing it with an electrical field.
  • a suitable gas for example may be xenon (Xe), or a xenon-argon mix.
  • a plasma 42 is generated in a manner to be described, and the plasma emits light (more generally photons of radiation of the desired wavelengths).
  • Collection optics 44 form at least one beam of radiation 46 that may be coupled to a optical fiber 48.
  • Fiber 48 delivers the radiation to the point where it is needed.
  • Reflective rather than refractive optics may be used.
  • Plasma 42 in this embodiment is generated by application of drive radiation 50 which is generated in this example by a laser 52.
  • Drive optics 54 focus the laser which reaches its narrowest point at the location where the plasma 42 is desired to be formed and maintained.
  • the laser 52 may be one of a number of different types of high power laser available today or in future. It may for example be a Nd:YAG laser, a C02 laser, a diode laser, a fiber laser.
  • Drive optics 54 is shown here as a simple lens, but can of course be more complex in practical embodiment. Reflective rather than refractive optics may be used. Further components may be provided to condition the laser radiation in its profile or spectral characteristics. A beam expander may be used, for example.
  • the laser radiation may be for example in infrared wavelengths, such as 700 to
  • the plasma 42 will typically be generating radiation at shorter wavelengths in the infrared, visible and/or ultraviolet bands, for example down to 200 nm or below. Among this plasma radiation are the desired wavelengths for use in the metrology apparatus or other application.
  • Electrodes 60 and 62 are provided with appropriate power and control circuitry (not shown), in order to ignite the plasma 42. These electrodes may be similar to those used in a conventional gas discharge lamp, but are used only during a start-up phase of operation.
  • the Z axis is aligned with an optical axis O.
  • the Y direction is aligned with the electrodes 60, 62.
  • the X axis is transverse to the electrodes, and normal to the plane of the diagram.
  • the apparatus can be constructed or mounted with these axes in any orientation that is convenient for its application. Note that there is no component obstructing the optical path from the plasma 42 to the collection optics 44 in the Z direction other than the radiation transparent material of the bulb 40. There is also in this example nothing obstructing the path of light in the X direction (not shown in this view).
  • plasma 42 may be elongate in form, having approximately the shape of a cylinder, or cigar.
  • the length of the cylinder is L and its diameter is d.
  • the real plasma will comprise a cloud of elongate form, centered on this cylindrical region.
  • Collection optics 44 is arranged with its optical axis O aligned with the longitudinal direction of the plasma, that is the Z direction in this example.
  • the area of the plasma 42 thus appears as ⁇ 2 /4, that is the area of one end of the cylinder.
  • the etendue of an optical source is broadly speaking the product of the area of the source (receiver) and its exit (entrance) angle.
  • the etendue of the collection optics 44 as with any imaging system, is the product of spot size times the square of its numerical aperture (NA2). The NA in turn is determined by the entrance angle.
  • the etendue of the radiating plasma is in general going to be larger than the etendue of the collection optics 44.
  • Collection optics 44 may be focused at a hypothetical source point 61 midway along the cylinder, as illustrated.
  • the length L of light emitting plasma region 42 may be on the order of a millimeter, say 0.5 to 5 mm.
  • the diameter d may be much smaller, in the range of say 0.01 to 2 mm, for example 0.1 to 1 mm.
  • the plasma 42 absorbs very little of the wanted radiation, so that photons emitted anywhere along the length L of the cylinder can travel in the entrance cone of collection optics 44 and into fiber 48. Therefore, compared with the transverse direction, the plasma appears brighter (greater luminous flux per unit area per unit solid angle) than when viewed in the transverse direction.
  • some laser driven light sources such as described in US 2011/204265 Al, seek to capture light emitted in the transverse direction
  • the photon source illustrated herein captures light emitted in the longitudinal direction to exploit the enhanced brightness and smaller extent of the plasma. Either capturing arrangement can be used in combination with the novel concepts disclosed herein.
  • a difficulty with the radiation source of Figure 4 is that the bulb 40 is usually in the form of a xenon (Xe) arc-discharge lamp whose design is not optimized for the present use.
  • a xenon (Xe) arc-discharge lamp which consists of a bulb made of glass in which pressurized xenon is placed, is used in a mode in which plasma is created by making an electric arc between the two electrodes 60,62.
  • the bulb 42 when the bulb 42 is being used in a laser-driven photon source apparatus such as illustrated in Figure 4 the bulb 42 tends to suffer from failures. This is thought to be due to thermal stresses set up in the glass and solarization of the glass due to UV radiation. Another difficulty is that the glass of the bulb 40 results in astigmatism; the glass of the bulb 40 is curved and so it behaves as a lens. Due to manufacturing tolerances, the glass of the bulb 40 is never perfectly as designed, so that astigmatism cannot reliably be accounted for in the optical system 44 downstream of the bulb 40.
  • Figure 5 shows a radiation source apparatus according to an embodiment of the invention. Note that plasma generation/excitation and collection/transport of the subsequent radiation follow the same structure and process as previously described in relation to Figure 4.
  • Figure 5 shows a container 400 of the present invention which replaces the bulb 40 of Figure 4.
  • the container 400 contains pressurized xenon (for example between 10 and 30 bar when cold and perhaps between 50 and 100 bar when hot).
  • the container 400 is an airtight (hermetically sealed) container.
  • the container 400 also comprises at least one radiation transmitting element, e.g. inlet radiation transmitting window 64 and/or outlet radiation transmitting element 65.
  • the container 400 comprises at least one filter component, e.g. filter components 66, 67.
  • filter components 66, 67 e.g. filter components 66, 67.
  • the radiation source does not necessarily have to take the form of that depicted and may take any other suitable form.
  • Drive radiation 50 may be focused by focusing optics 54 onto plasma 42, entering the container 400 via inlet radiation transmitting element 64. Radiation generated by plasma 42 may exit the container 400 via outlet radiation transmitting element 65, to be collected by collection optics 44.
  • filter components 66 block ultraviolet radiation (10-400 nm wavelength radiation) exiting the container 400 through inlet radiation transmitting element 64.
  • filter components 67 may block ultraviolet and/or infrared (700-1000 nm wavelength) radiation exiting the container 400 through outlet radiation transmitting element 65.
  • the filter components 66, 67 may be in the form of a coating.
  • the coating may be on the side of the radiation transmitting element 64, 65 facing the plasma 42 or on the opposite side to the plasma 42.
  • An advantage of the filter component 66, 67 being on the side of the plasma 42 is that the filter component 66, 67 thereby protects the radiation transmitting element 64, 65 from the radiation which is filtered out. If UV radiation is filtered out, this can protect the radiation transmitting element 64, 65 from solarization if the element is susceptible to solarization by UV radiation.
  • Filter components 66, 67 may be provided in the optical path and made of suitable materials with variable thickness, fixed by the required wavelengths. Filter components 66, 67 may also be integrated with other components of the collection optics 44.
  • the filter components 66, 67 and radiation transmitting elements 64, 65 may be incorporated in a single component.
  • the radiation transmitting element 64, 65 may be comprised of a material which absorbs radiation in the desired wavelength range.
  • a radiation transmitting element comprising Ti0 2 (e.g. glass or other material transparent to radiation coated with Ti0 2 or glass or other material transparent to radiation doped with Ti0 2 ) may be used.
  • the output radiation transmitting element 65 may be comprised of suprasil (RTM), a synthetic fused silica available from Heraeus Quartzglass, Hanau, Germany.
  • Radiation transmitting elements 64 and 65 should be gastight and made of suitable coated/uncoated materials.
  • the radiation transmitting elements 64, 65 may also be any size, shape or thickness and/or may be flat/curved.
  • at least one of the radiation transmitting elements 64, 65 comprises a plane parallel plate. This is advantageous as the problem of astigmatism with a bulb 40 such as in Figure 4 is solved.
  • the container 400 is made of a size and/or shape such that, in use, the distance between the center 61 of the plasma 42 and the radiation transmitting windows 65, 66 is much larger than that of bulb 40. This is advantageous because any thermal stresses set up on the radiation transmitting windows 64, 65 will be much lower than those in the bulb 40 and the lifetime of the container 400 will therefore be much greater than that of bulb 40.
  • the center 61 of the plasma 42 is directly between and equidistant from the tips of the electrodes 60, 62 and/or at the focus point of the drive optics 54.
  • Prior art containers in the form of a bulb 40 are substantially spherical in
  • the distance of walls of the bulb (equivalent to the light transmitting windows 65, 66) to the center 61 of the plasma 42 is about equal to the radius of the sphere of the bulb 40. Therefore, in prior art bulbs the distance from the center 61 of the plasma 42 to the light transmitting window 65, 66 is about ⁇ V ⁇ — where V is the
  • the inventors have appreciated that the lifetime of the bulb can be significantly increased by using an arrangement in which the center 61 of the plasma 42 is positioned further from the walls on which the plasma emitted radiation impinges which are sensitive to plasma emitted radiation. In an embodiment this is achieved by having a non-spherically shaped container (e.g. an elongate container) in which side walls, at least in a central portion, are comprised of a material more able to withstand plasma emitted radiation impinging on them than the radiation transmitting elements 64, 65.
  • the container 400 may contain a volume of gas which extends in the longitudinal direction with the optical axis O.
  • a central plasma surrounding volume 600 and on one side a inlet volume 610 and the other side an outlet volume 620.
  • the plasma 42 is in the plasma surrounding volume 600.
  • the driving radiation 50 passes through the inlet volume 610.
  • the plasma emitted radiation passes through the outlet volume 620.
  • the plasma surrounding volume 600 substantially surrounds the plasma 42 except for radiation and inlet and outlet openings 601, 602 and is for containing gas surrounding the plasma 42.
  • the size of the plasma surrounding volume 600 is similar to that of prior art bulb volumes.
  • the volume of the plasma surrounding volume 600 is less than 200000 mm 3 preferably less than 100000 mm 3 or even less than 1000 mm 3 or even less than 100 mm 3 . This has the advantage of being quite a small volume so that the plasma 42 is stable and the gas surrounding the plasma 42 does not cool the plasma 42 too much as might occur if the plasma surrounding volume were larger.
  • an average cross sectional area in a plane perpendicular to the axis O of the plasma surrounding volume 600 is smaller than the average cross sectional area of the inlet volume 610 and/or outlet volume 620.
  • the center 61 of the plasma 42 is substantially further from the outlet radiation transmitting element 66 and/or inlet radiation transmitting element 65 as from the nearest wall of the container 400.
  • the center 61 of the plasma 42 is at least three times (preferably at least six times) as far from the outlet radiation transmitting element 66 and/or inlet radiation transmitting element 65 as from the nearest wall of the container 400.
  • the walls of the container 400 defining the plasma surrounding volume 600 (which are nearest the center 61 of the plasma 42 and do not include the electrodes 60, 62) define a much smaller volume than the total volume of the container 400. This means that the plasma 42 is stable whilst the inlet and outlet radiation transmitting elements 65, 66 are protected from intense plasma emitted radiation.
  • V is the volume of the plasma surrounding volume 600.
  • At least one of a distance between a center of the plasma and said inlet radiation transmitting element and a distance between the center of the plasma and said outlet radiation transmitting element at least 6 times liV ⁇ — .
  • the plasma 42 is formed at a location at least 10 mm from one or both of the inlet and outlet radiation transmitting elements 64, 65.
  • at least one of the inlet and outlet radiation transmitting elements 64, 65 is positioned at least 20 mm, more desirably at least 30 mm from the plasma 42 or even more than 35, 40 or 50 mm.
  • the container 400 comprises an axis of symmetry O extending in the z
  • the plasma 42 is formed on the axis of symmetry O.
  • the inlet and outlet radiation transmitting elements 64, 65 are positioned perpendicular to the axis of symmetry O, which defines a longitudinal direction.
  • Driving radiation 50 travels substantially parallel to the longitudinal axis O. Radiation emitted by the plasma 42 exits through the outlet radiation transmitting element 65 and is substantially parallel to the axis of symmetry O.
  • the drive optics 54 and/or collection optics 44 are at least partly formed by the inlet radiation transmitting element 64 and outlet radiation transmitting element 65 respectively. That is, one or both the radiation transmitting elements 64, 65 may not be in the form of a plane parallel plate. However, ensuring that the radiation transmitting elements 64, 65 are plane parallel plates makes manufacture of the container 400 less problematic.
  • the container 400 comprises at least two electrodes 60, 62.
  • the electrodes 60, 62 are connected to The electrodes 60, 62.
  • a body 410 of the container 400 is illustrated as being comprised of a solid material. This is not necessarily the case.
  • the body 410 (particularly the walls defining the plasma surrounding volume 600, e.g. the central portion of the container 400 walls) is made of a material more able than the radiation transmitting elements 64, 65 to withstand irradiation by plasma emitted radiation.
  • the internal surface of the body 410 of the container 400 may be made of a reflective material. This can aid in maintaining the temperature of the plasma 42 by reflection of radiation emitted by the plasma 42 back to the plasma 42.
  • the container 400 may have an internal volume
  • a central portion between the two truncated cones may be cylindrical, spherical, ovoid etc. and designed to hold the plasma 42.
  • the walls of airtight container 400 may be made of suitable materials which are able to block unwanted radiation (or all radiation), for example, materials which block UV radiation generated by the plasma 42. Furthermore, container 400 may be of any dimension, shape and wall thickness to meet the application requirements.
  • the container 400 is airtight and ultraviolet light is filtered out from the output radiation 44 (example.e. at radiation transmitting element 64, 65), ozone produced by ultraviolet light acting on air advantageously does not occur.
  • the plasma extends longitudinally in what is depicted as the Y direction, between the igniting electrodes, in the illustrated source the plasma in normal operation is arranged so that rays in the longitudinal direction are not obscured, and can be captured by the collection optics 44.
  • the plasma extends in what is depicted as the Z direction, this is obscured by the driving laser optics, and the usable light is captured by a curved mirror, after being emitted in the X and Y directions from the plasma.
  • many prior examples rely on capturing the photons emitted transversely from the plasma.
  • Embodiments of the invention may also or alternatively rely on capturing the photons emitted transversely from the plasma.
  • the intensity profile of the radiation emitted by the plasma source might not be perfectly uniform across the field of view of collection optics 44. While constraints on the plasma dimensions are relaxed as described above, still the entrance NA of collection optics 44 should be reasonably uniformly filled with radiation. The larger the aspect ratio L/d of the plasma, the smaller the etendue will be in which the radiation is uniformly distributed. Mixing of the light to make it more homogeneous may be desired, for example when the radiation source apparatus is used to deliver a homogeneous light field across aperture 13 in the apparatus of Figure 3. Sufficient mixing may occur naturally within the fiber 48, or additional measures may be taken.
  • optical properties of the inlet and outlet radiation transmitting elements 64, 65 should be good enough at the key locations that they do not degrade the quality of the drive laser beam or the rays emanating from plasma 42 to collection optics 44.
  • the optical properties of the inlet and outlet radiation transmitting elements 64, 65 and filters 66, 67, should of course be taken into account in designing and setting up the collection optics 44 and focusing optics 54.
  • Functional elements of collection optics 44 and focusing optics 54 can be placed inside container 400 if desired, and/or may be integrated with the wall of the container 400.
  • the container 400 is substantially rotationally symmetric around the longitudinal axis O.
  • a rotator 700 may be provided to rotate the container 400 about the longitudinal axis O as illustrated by arrow 710. This is advantageous as any uneven heating loads due to the plasma 42 which are generated (for example due to convection of the gas in the container 400) can be made to have a equal effect around the circumference of the container 400. As a result large thermal gradients can be avoided. Additionally this embodiment makes use of the variation in density in the gas in the container 400. The hottest gas, namely that in the plasma 42, will be least dense and other parts of the gas not formed in the plasma 42 will be more dense. The hottest parts of the gas not in the plasma 42 will have a lower density than the cooler parts.
  • the cold and more dense gas will be pushed to the outside of the container 400 and the lighter gas and plasma 42 will concentrate in the center along the longitudinal axis O.
  • This has the effect of decreasing the plasma 42 size and therefore has a positive effect on the plasma 42 intensity.
  • the size of the plasma 42 will be reduced and it will act more like a point source thereby increasing the overall efficiency of the radiation source.
  • any convection in the gas in the container 400 is not as strong thereby resulting in warmer plasma and lower thermal gradients within the container 400.
  • the plasma 42 will advantageously be kept hotter due to the presence of the hottest gas being next to the plasma 42.
  • a suitable speed for rotation may be more than 100 revolutions per minute, for example above 500 revolutions per minute, perhaps as much as 1000 revolutions per minute or more.
  • lithographic apparatus in the manufacture of ICs
  • the lithographic apparatus described herein may have other applications, such as the manufacture of integrated optical systems, guidance and detection patterns for magnetic domain memories, flat-panel displays, liquid-crystal displays (LCDs), thin-film magnetic heads, etc.
  • the invention may be applied in industrial processing applications quite separate from lithography. Examples might be in production of optical components, automotive manufacture, construction - any number of applications where object data exists in the form of measurements made with a certain spatial distribution over the product.
  • the set of measurements that is subjected to multivariate analysis can be
  • imprint lithography a topography in a patterning device defines the pattern created on a substrate.
  • the topography of the patterning device may be pressed into a layer of resist supplied to the substrate whereupon the resist is cured by applying electromagnetic radiation, heat, pressure or a combination thereof.
  • the patterning device is moved out of the resist leaving a pattern in it after the resist is cured
  • electromagnetic radiation including ultraviolet (UV) radiation (e.g., having a wavelength of or about 365, 355, 248, 193, 157 or 126 nm) and extreme ultra-violet (EUV) radiation (e.g., having a wavelength in the range of 5-20 nm), as well as particle beams, such as ion beams or electron beams.
  • UV radiation e.g., having a wavelength of or about 365, 355, 248, 193, 157 or 126 nm
  • EUV extreme ultra-violet
  • particle beams such as ion beams or electron beams.
  • the term radiation in the context of the driving system may also encompass microwave radiation.
  • the term "lens”, where the context allows, may refer to any one or combination of various types of optical components, including refractive, reflective, magnetic, electromagnetic and electrostatic optical components.

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Abstract

L'invention concerne un appareil source de rayonnement qui comporte : un contenant (400) devant être mis sous pression à l'aide d'un milieux gazeux dans lequel un plasma, qui émet un rayonnement émis par plasma, est généré suite à l'excitation du milieu gazeux par un rayonnement d'attaque (50), ledit contenant étant utilisable (66, 67) pour éliminer sensiblement le rayonnement dont la longueur d'onde est de 10 à 400 nm dudit rayonnement émis par plasma avant que ledit rayonnement émis par plasma sorte dudit contenant en tant que rayonnement émis. Dans un mode de réalisation, le contenant comporte : un élément d'admission de transmission de rayonnement (64) utilisable pour transmettre ledit rayonnement d'attaque depuis l'extérieur dudit contenant vers l'intérieur dudit contenant, et un élément de sortie de transmission de rayonnement (65) utilisable pour transmettre au moins une partie dudit rayonnement émis par plasma depuis l'intérieur dudit contenant vers l'extérieur dudit contenant en tant que rayonnement émis, ledit élément d'admission de transmission de rayonnement et/ou ledit élément de sortie de transmission de rayonnement comportant une plaque parallèle au plan.
PCT/EP2014/074659 2013-12-13 2014-11-14 Source de rayonnement, appareil de métrologie, système lithographique et procédé de fabrication de dispositifs WO2015086258A1 (fr)

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US15/103,721 US9924585B2 (en) 2013-12-13 2014-11-14 Radiation source, metrology apparatus, lithographic system and device manufacturing method
CN201480067916.7A CN105814662B (zh) 2013-12-13 2014-11-14 辐射源、量测设备、光刻系统和器件制造方法
KR1020167018014A KR101953712B1 (ko) 2013-12-13 2014-11-14 방사선 소스, 계측 장치, 리소그래피 시스템 및 디바이스 제조 방법
IL245915A IL245915B (en) 2013-12-13 2016-05-30 Irradiation source, metrological device, lithographic system and method for preparing the device
US15/888,362 US10420197B2 (en) 2013-12-13 2018-02-05 Radiation source, metrology apparatus, lithographic system and device manufacturing method

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US9924585B2 (en) 2018-03-20
US20160316550A1 (en) 2016-10-27
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TW201523169A (zh) 2015-06-16
CN105814662A (zh) 2016-07-27

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